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Kovac, John

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Kovac

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Kovac, John

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Now showing 1 - 10 of 11
  • Publication

    Parity Violation Constraints Using Cosmic Microwave Background Polarization Spectra from 2006 and 2007 Observations by the QUaD Polarimeter

    (American Physical Society, 2009) Wu, E.Y.S.; Ade, P.; Bowden, M.; Brown, M.L.; Cahill, G.; Castro, P.G.; Church, S.; Culverhouse, T.; Ganga, K.; Gear, W.K.; Gupta, S.; Hinderks, J.; Kovac, John; Lange, A.E.; Leitch, E.; Melhusish, S.J.; Memari, Y.; Murphy, J.A.; Orlando, A.; Piccirillo, L.; Pryke, C.; Rajguru, N.; Rusholme, B.; Schwarz, R.; O'Sullivan, C.; Taylor, A.N.; Thompson, K.L.; Turner, A.H.; Zemcov, M.; Bock, J.; Friedman, R B

    We constrain parity-violating interactions to the surface of last scattering using spectra from the QUaD experiment’s second and third seasons of observations by searching for a possible systematic rotation of the polarization directions of cosmic microwave background photons. We measure the rotation angle due to such a possible ‘‘cosmological birefringence’’ to be (0.55^{\circ} \pm 0.82^{\circ}) (random) (\pm 0.5^{\circ}) (systematic) using QUaD’s 100 and 150 GHz temperature-curl and gradient-curl spectra over the spectra over the multipole range 200 <(\ell)< 2000, consistent with null, and constrain Lorentz-violating interactions to <2 (\times) 10(^ {-43}) GeV (68% confidence limit). This is the best constraint to date on electrodynamic parity violation on cosmological scales.

  • Publication

    QUaD: A High-Resolution Cosmic Microwave Background Polarimeter

    (IOP Publishing, 2009) Hinderks, James R.; Ade, Peter; Bock, James; Bowden, Melanie; Brown, Michael L.; Cahill, Gary; Carlstrom, John E.; Castro, Patricia G.; Church, Sarah; Culverhouse, Thomas; Friedman, Robert; Ganga, Ken; Gear, Walter K.; Gupta, Sujata; Harris, J.; Haynes, V.; Keating, Brian G.; Kovac, John; Kirby, E.; Lange, Andrew E.; Leitch, Erik; Mallie, Olivier E.; Melhuish, Simon J.; Memari, Yasin; Murphy, J. Anthony; Orlando, Angiola; Schwarz, Robert; O'Sullivan, Creidhe; Piccirillo, Lucio; Pryke, Clement; Rajguru, Nutan; Rusholme, Ben; Taylor, Andrew N.; Thompson, Keith L.; Tucker, Carole; Turner, Abigail H.; Wu, Ed Y. S.; Zemcov, Michael

    We describe the QUaD experiment, a millimeter-wavelength polarimeter designed to observe the cosmic microwave background (CMB) from a site at the South Pole. The experiment comprises a 2.64 m Cassegrain telescope equipped with a cryogenically cooled receiver containing an array of 62 polarization-sensitive bolometers. The focal plane contains pixels at two different frequency bands, 100 GHz and 150 GHz, with angular resolutions of 5' and 3'.5, respectively. The high angular resolution allows observation of CMB temperature and polarization anisotropies over a wide range of scales. The instrument commenced operation in early 2005 and collected science data during three successive Austral winter seasons of observation

  • Publication

    Second and Third Season QUaD Cosmic Microwave Background Temperature and Polarization Power Spectra

    (IOP Publishing, 2009) Pryke, Clement; Ade, Peter; Bock, James; Bowden, Melanie; Brown, Michael L.; Cahill, Gary; Castro, Patricia G.; Church, Sarah; Culverhouse, Thomas; Friedman, Robert; Ganga, Ken; Gear, Walter K.; Gupta, Sujata; Hinderks, James; Kovac, John; Lange, Andrew E.; Leitch, Erik; Melhuish, Simon J.; Memari, Yasin; Murphy, J. Anthony; Orlando, Angiola; Schwarz, Robert; O'Sullivan, Creidhe; Piccirillo, Lucio; Rajguru, Nutan; Rusholme, Ben; Taylor, Andrew N.; Thompson, Keith L.; Turner, Abigail H.; Wu, Ed Y. S.; Zemcov, Michael B.

    We report results from the second and third seasons of observation with the QUaD experiment. Angular power spectra of the cosmic microwave background are derived for both temperature and polarization at both 100 GHz and 150 GHz, and as cross-frequency spectra. All spectra are subjected to an extensive set of jackknife tests to probe for possible systematic contamination. For the implemented data cuts and processing technique such contamination is undetectable. We analyze the difference map formed between the 100 and 150 GHz bands and find no evidence of foreground contamination in polarization. The spectra are then combined to form a single set of results which are shown to be consistent with the prevailing LCDM model. The sensitivity of the polarization results is considerably better than that of any previous experiment—for the first time multiple acoustic peaks are detected in the E-mode power spectrum at high significance.

  • Publication

    Improved Measurements of the Temperature and Polarization of the Cosmic Microwave Background from QUaD

    (IOP Publishing, 2009) Brown, M. L.; Ade, P.; Bock, J.; Bowden, M.; Cahill, G.; Castro, P. G.; Church, S.; Culverhouse, T.; Friedman, R. B.; Ganga, K.; Gear, W. K.; Gupta, S.; Hinderks, J.; Kovac, John; Lange, A. E.; Leitch, E.; Melhuish, S. J.; Memari, Y.; Murphy, J. A.; Orlando, A.; Sullivan, C. O; Piccirillo, L.; Pryke, C; Rajguru, N.; Rusholme, B.; Schwarz, R.; Taylor, A. N.; Thompson, K. L.; Turner, A. H.; Wu, E. Y. S.; Zemcov, M.

    We present an improved analysis of the final data set from the QUaD experiment. Using an improved technique to remove ground contamination, we double the effective sky area and hence increase the precision of our cosmic microwave background (CMB) power spectrum measurements by ~30% versus that previously reported. In addition, we have improved our modeling of the instrument beams and have reduced our absolute calibration uncertainty from 5% to 3.5% in temperature. The robustness of our results is confirmed through extensive jackknife tests, and by way of the agreement that we find between our two fully independent analysis pipelines. For the standard six-parameter ΛCDM model, the addition of QUaD data marginally improves the constraints on a number of cosmological parameters over those obtained from the WMAP experiment alone. The impact of QUaD data is significantly greater for a model extended to include either a running in the scalar spectral index, or a possible tensor component, or both. Adding both the QUaD data and the results from the Arcminute Cosmology Bolometer Array Receiver experiment, the uncertainty in the spectral index running is reduced by ~25% compared to WMAP alone, while the upper limit on the tensor-to-scalar ratio is reduced from r < 0.48 to r < 0.33 (95% c.l.). This is the strongest limit on tensors to date from the CMB alone. We also use our polarization measurements to place constraints on parity-violating interactions to the surface of last scattering, constraining the energy scale of Lorentz violating interactions to <1.5 × 10–43 GeV (68% c.l.). Finally, we place a robust upper limit on the strength of the lensing B-mode signal. Assuming a single flat band power between ℓ = 200 and ℓ = 2000, we constrain the amplitude of B-modes to be <0.57 μK2 (95% c.l.).

  • Publication

    Small angular scale measurements of the cosmic microwave background temperature power spectrum from QUaD

    (IOP Publishing, 2009) Friedman, R. B.; Ade, P.; Bock, J.; Bowden, M.; Brown, M. L.; Cahill, G.; Castro, P. G.; Church, S.; Culverhouse, T.; Ganga, K.; Gear, W. K.; Gupta, S.; Hinderks, J.; Kovac, John; Lange, A. E.; Leitch, E.; Melhuish, S. J.; Memari, Y.; Murphy, J. A.; Orlando, A.; O'Sullivan, C.; Piccirillo, L.; Pryke, C; Rajguru, N.; Rusholme, B.; Schwarz, R.; Taylor, A. N.; Thompson, K. L.; Turner, A. H.; Wu, E. Y. S.; Zemcov, M.

    We present measurements of the cosmic microwave background (CMB) radiation temperature anisotropy in the multipole range 2000 << 3000 from the QUaD telescope’s second and third observing seasons. After masking the brightest point sources our results are consistent with the primary ΛCDM expectation alone. We estimate the contribution of residual (un-masked) radio point sources using a model calibrated to our own bright source observations, and a full simulation of the source finding and masking procedure. Including this contribution slightly improves the χ2. We also fit a standard Sunyaev–Zel’dovich (SZ) template to the bandpowers and see no strong evidence of an SZ contribution, which is as expected for σ8 ≈ 0.8.

  • Publication

    BICEP2/SPUD: searching for inflation with degree scale polarimetry from the South Pole

    (SPIE, 2008) Nguyen, Hien Trong; Kovac, John; Ade, Peter; Aikin, Randol; Benton, Steve; Bock, James; Brevik, Justus; Carlstrom, John; Dowell, Darren; Duband, Lionel; Golwala, Sunil; Halpern, Mark; Hasslefield, Matthew; Irwin, Kent; Jones, William; Kaufman, Jonathan; Keating, Brian; Kuo, Chao-Lin; Lange, Andrew; Matsumura, Tomotake; Netterfield, Barth; Pryke, Clem; Ruhl, John; Sheehy, Chris; Sudiwala, Rashmi

    BICEP2/SPUD is the new powerful upgrade of the existing BICEP1 experiment, a bolometric receiver to study the polarization of the cosmic microwave background radiation, which has been in operation at the South Pole since January 2006. BICEP2 will provide an improvement up to 10 times mapping speed at 150 GHz compared to BICEP1, using the same BICEP telescope mount. SPUD, a series of compact, mechanically-cooled receivers deployed on the DASI mount at the Pole, will provide similar mapping speed in to BICEP2 in three bands, 100, 150, and 220 GHz. The new system will use large TES focal plane arrays to provide unprecedented sensitivity and excellent control of foreground contamination.

  • Publication

    Microfabrication and Device Parameter Testing of the Focal Plane Arrays for the Spider and BICEP2?Keck CMB Polarimeters

    (2009) Bonetti, J. A.; Turner, A. D.; Kenyon, M.; Orlando, A.; Brevik, J. A.; Trangsrud, A.; Sudiwala, R.; LeDuc, H. G.; Nguyen, H. T.; Day, P. K.; Bock, J. J.; Golwala, S. R.; Sayers, J.; Kovac, John; Lange, A. E.; Jones, W. C.; Kuo, C. L; Young, Betty; Cabrera, Blas; Miller, Aaron

    Spider and BICEP2/Keck are projects to study the polarization of the cosmic microwave background (CMB). The focal planes for both require large format arrays of superconducting transition edge sensors (TES's). A major challenge for these projects is fabricating arrays with high uniformity in device parameters. A microfabrication process is described that meets this challenge. The results from device testing are discussed. Each focal plane is composed of 4 square wafers (tiles), and each wafer contains 128 membrane-isolated, polarization-sensitive, antenna-coupled TES's. After processing, selected wafers are pre-screened in a quick-turn-around, cryogen-free, ^He fridge. The pre-screening is performed with a commercial resistance bridge and measures transition temperatures (Tc) and normal state resistances (R„). After pre-screening, 4 tiles at a time are fully characterized in a testbed employing a SQUID readout and SQUID mulitplexing. The tests demonstrate the values of Tc, RB, thermal conductance, g, and the standard deviations of each, across a wafer and from wafer to wafer, are within design specifications.

  • Publication

    Cosmological Parameters From the Quad Cmb Polarization Experiment

    (IOP Publishing, 2009) Castro, P. G.; Ade, P.; Bock, J.; Bowden, M.; Brown, M. L.; Cahill, G.; Church, S.; Culverhouse, T.; Friedman, R. B.; Ganga, K.; Gear, W. K.; Gupta, S.; Hinderks, J.; Kovac, John; Lange, A. E.; Leitch, E.; Melhuish, S. J.; Memari, Y.; Murphy, J. A.; Orlando, A.; Pryke, C; Schwarz, R.; O, C.; Piccirillo, L.; Rajguru, N.; Rusholme, B.; Taylor, A. N.; Thompson, K. L.; Turner, A. H.; Wu, E. Y. S.; Zemcov, M.

    In this paper, we present a parameter estimation analysis of the polarization and temperature power spectra from the second and third season of observations with the QUaD experiment. QUaD has for the first time detected multiple acoustic peaks in the E-mode polarization spectrum with high significance. Although QUaD-only parameter constraints are not competitive with previous results for the standard six-parameter ΛCDM cosmology, they do allow meaningful polarization-only parameter analyses for the first time. In a standard six-parameter ΛCDM analysis, we find the QUaD TT power spectrum to be in good agreement with previous results. However, the QUaD polarization data show some tension with ΛCDM. The origin of this 1σ–2σ tension remains unclear, and may point to new physics, residual systematics, or simple random chance. We also combine QUaD with the five-year WMAP data set and the SDSS luminous red galaxies 4th data release power spectrum, and extend our analysis to constrain individual isocurvature mode fractions, constraining cold dark matter density, αcdmi < 0.11 (95% confidence limit (CL)), neutrino density, αndi < 0.26 (95% CL), and neutrino velocity, αnvi < 0.23 (95% CL), modes. Our analysis sets a benchmark for future polarization experiments.

  • Publication

    First Season QUaD CMB Temperature and Polarization Power Spectra

    (IOP Publishing, 2008) Ade, P.; Bock, J.; Bowden, M.; Brown, M. L.; Cahill, G.; Carlstrom, J. E.; Castro, P. G.; Church, S.; Culverhouse, T.; Friedman, R.; Ganga, K.; Gear, W. K.; Hinderks, J.; Kovac, John; Lange, A. E.; Leitch, E.; Melhuish, S. J.; Murphy, J. A.; Orlando, A.; Schwarz, R.; O’Sullivan, C.; Piccirillo, L.; Pryke, C.; Rajguru, N.; Rusholme, B.; Taylor, A. N.; Thompson, K. L.; Wu, E. Y. S.; Zemcov, M.

    QUaD is a bolometric CMB polarimeter sited at the South Pole, operating at frequencies of 100 and 150 GHz. In this paper we report preliminary results from the first season of operation (austral winter 2005). All six CMB power spectra are presented derived as cross spectra between the 100 and 150 GHz maps using 67 days of observation in a low foreground region of approximately 60 square degrees. This data is a small fraction of the data acquired to date. The measured spectra are consistent with the LCDM cosmological model. We perform jackknife tests which indicate that the observed signal has negligible contamination from instrumental systematics. In addition by using a frequency jackknife we find no evidence for foreground contamination.

  • Publication

    The Origin of the Universe as Revealed Through the Polarization of the Cosmic Microwave Background

    (2009) Dodelson, S.; Easther, R.; Hanany, S.; McAllister, L.; Meyer, S.; Page, L.; Ade, P.; Amblard, A.; Ashoorioon, A.; Balbi, C.; Bartlett, J.; Bartolo, N.; Baumann, D.; Beltran, M.; Benford, D.; Birkinshaw, M.; Bock, J.; Bond, D.; Borrill, J.; Bouchet, F.; Bridges, M.; Bunn, E.; Calabrese, E.; Cantalupo, C.; Caramete, A.; Carbone, C.; Carroll, S.; Chatterjee, S.; Chen, Xingang; Church, S.; Chuss, D.; Contaldi, C.; Cooray, A.; Creminelli, P.; Das, S.; De Bernardis, F.; Delabrouille, J.; Desert, F.; Devlin, M.; Dickinson, C.; Dicker, S.; DiPirro, M.; Dobbs, M.; Dore, O.; Dotson, J.; Dunkley, J.; Dvorkin, Cora; Eriksen, H.; Falvella, M.; Finley, D.; Finkbeiner, Douglas; Fixsen, D.; Flauger, R.; Fossalba, P.; Fowler, J.; Galli, S.; Gates, E.; Gear, W.; Giraud-Heraud, Y.; Krzysztof, G.; Greene, B.; Gruppuso, A.; Gundersen, J.; Halpern, M.; Hamilton, J.; Hazumi, M.; Hernandez-Monteagudo, C.; Hertzberg, M.; Hinshaw, G.; Hirata, C.; Hivon, E.; Holman, R.; Holmes, W.; Hu, W.; Hubmayr, J.; Huffenberger, K.; Hui, H.; Hui, L.; Irwin, K.; Jackson, M.; Jaffe, A.; Johnson, B.; Johnson, D.; Jones, W.; Kachru, S.; Kadota, K.; Kaplan, J.; Kaplinghat, W.; Keating, B.; Keskitalo, R.; Khoury, J.; Kinney, W.; Kisner, T.; Knox, T.; Kodama, H.; Kogut, A.; Komatsu, E.; Kosowsky, A.; Kovac, John; Krauss, L.; Kurki-Suonio, H.; Lamarre, J.; Landau, S.; Lawrenece, C.; Leach, S.; Leblond, L.; Lee, A.; Leitch, E.; Leonardi, R.; Lesgourgues, J.; Liddle, A.; Lim, E.; Limon, M.; LoVerde, M.; Lubin, P.; Lunghi, E.; Lykken, J.; MacTavish, C.; Magalhaes, A.; Maino, D.; Martin, V.; Matarrese, S.; Mather, J.; Mathur, H.; Matsumura, T.; Meerburg, P.; Melchiorri, A.; Mersini-Houghton, L.; Miller, A.; Milligan, M.; Moodley, K.; Neimack, M.; Nguyen, H.; Nicolis, A.; O'Dwyer, I.; Olinto, A.; Pagano, L.; Paher, E.; Partridge, B.; Pearson, T.; Peiris, H.; Peloso, M.; Piacentini, F.; Piat, M.; Piccirillo, L.; Pierpaoli, E.; Pietrobon, D.; Pisano, G.; Pogosian, L.; Pogosyan, D.; Ponthieu, N.; Popa, L.; Pryke, C; Raeth, C.; Ray, S.; Reichardt, C.; Riccardi, S.; Richards, P.; Riotto, A.; Rocha, G.; Ruhl, J.; Rusholme, B.; Scherrer, R.; Scoccola, C.; Scott, D.; Sealfon, C.; Sefusatti, E.; Sehgal, N.; Seiffert, M.; Senatore, L.; Serra, P.; Shandera, S.; Shimon, M.; Shirron, P.; Sievers, J.; Silk, J.; Sigurdson, K.; Silverberg, R.; Silverstein, E.; Staggs, S.; Starkman, G.; Stebbins, A.; Stivoli, F.; Stompor, R.; Sugiyama, N.; Swetz, D.; Tegmark, M.; Tartari, A.; Timbie, P.; Titov, M.; Tristram, M.; Trodden, M.; Tucker, G.; Urrestilla, J.; Veneziani, M.; Verde, L.; Vieira, J.; Walker, T.; Wands, D.; Watson, S.; Weinberg, S.; Weiss, R.; Wandelt, B.; Winstein, B.; Wollack, E.; Wyman, M.; Yadav, A.; Won Yoon, K.; Zahn, O.; Zaldarriaga, M.; Zemcov, M.; Zwart, J.

    Modern cosmology has sharpened questions posed for millennia about the origin of our cosmic habitat. The age-old questions have been transformed into two pressing issues primed for attack in the coming decade: • How did the Universe begin? The current cosmological paradigm successfully explains how the majestic structure observed in the Universe today grew out of small ripples in the density of matter. What is the physical origin of the primordial seeds which are ultimately responsible for the existence of galaxies, stars, planets, and people in the Universe? It is natural to expect (and many theories predict) that whatever produced the density ripples also produced gravity waves – undulations in the fabric of space-time which travel at the speed of light. Does the Universe contain a spectrum of primordial gravity waves produced by the same mechanism which produced the ripples in the density? • What physical laws govern the Universe at the highest energies? All explanations for the seeds of structure rely on physics at energies far beyond those probed by, e.g., CERN’s Large Hadron Collider. Experiments probing these seeds therefore may provide information about new particles, forces, or perhaps even extra dimensions of space that are visible only at the highest energies. The clearest window onto these questions is the pattern of polarization in the Cosmic Microwave Background (CMB), which is uniquely sensitive to primordial gravity waves. A detection of the special pattern produced by gravity waves would be not only an unprecedented discovery, but also a direct probe of physics at the earliest observable instants of our Universe. Experiments which map CMB polarization over the coming decade will lead us on our first steps towards answering these age-old questions.